with the parameters \(A_i\) , \(B_i\)  and \(\alpha _i\)  fitted to the data of the nucleon's electromagnetic form factors.
The forward limit of the GPD \(H^a\)  is given by the flavor-a parton density, \(q^a(x)\)  which is taken from
[1]}. Since the forward limit of \(E^a\)  is not accessible in deep-inelastic scattering it is,
therefore, to be determined in the form factor analysis, too. The most prominent feature of the GPDs,
parameterized as in (REF ) and (REF ), is the strong \(x - t\)  correlation
[2]}, [3]}: The GPDs at small \(x\)  control the behavior of their associated flavor form factors at
small \(-t\)  whereas large \(x\)  determine their large \(-t\)  behavior. The flavor
form factors \(R_V^a\)  and \(R_T^a\)  are evaluated from the GPDs (REF ), (REF ). These
flavor form factors have also been used in wide-angle Compton scattering [3]}.
